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arXiv 1809.02248math-phmath.MP
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非线性振子的整体与局部超可积性

Global versus local superintegrability of nonlinear oscillators

Stephen C. Anco, Angel Ballesteros, Maria Luz Gandarias

摘要:

哈密顿微分方程组的刘维尔(超)可积性是基于运动的全局定义常数的存在性,而李点对称性提供了守恒积分的局部方法。因此,研究李点对称在什么意义上可以用来提供关于给定哈密顿系统的超可积性的信息似乎是很自然的。二维振子和中心力问题作为基准的例子来表明,标准李点对称性和超可积性之间的关系既不简单,也不普遍。一般来说,超可积性与变分动力学对称代数的大小或结构无关。然而,对于一个给定的哈密顿系统,所有的第一积分可以通过标准点对称方法的扩展来获得,该方法被应用于描述具有非常曲率和球对称空间上的粒子运动的超可积非线性振子。

英文摘要:

Liouville (super)integrability of a Hamiltonian system of differential equations is based on the existence of globally well-defined constants of the motion, while Lie point symmetries provide a local approach to conserved integrals. Therefore, it seems natural to investigate in which sense Lie point symmetries can be used to provide information concerning the superintegrability of a given Hamiltonian system. The two-dimensional oscillator and the central force problem are used as benchmark examples to show that the relationship between standard Lie point symmetries and superintegrability is neither straightforward nor universal. In general, it turns out that superintegrability is not related to either the size or the structure of the algebra of variational dynamical symmetries. Nevertheless, all of the first integrals for a given Hamiltonian system can be obtained through an extension of the standard point symmetry method, which is applied to a superintegrable nonlinear oscillator describing the motion of a particle on a space with non-constant curvature and spherical symmetry.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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